{"title":"用宇宙双折射解析负有效中微子质量参数","authors":"Toshiya Namikawa","doi":"10.1103/qgnn-6hsf","DOIUrl":null,"url":null,"abstract":"The recent measurement of baryonic acoustic oscillations by the Dark Energy Spectroscopic Instrument reveals a mild tension with observations of the cosmic microwave background (CMB) within the standard Λ</a:mi></a:math> cold dark matter (<d:math xmlns:d=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><d:mi mathvariant=\"normal\">Λ</d:mi><d:mi>CDM</d:mi></d:math>) cosmological model. This discrepancy leads to a preference for a total neutrino mass that is lower than the minimum value inferred from neutrino oscillation experiments. Alternatively, this tension can be eased within <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi mathvariant=\"normal\">Λ</g:mi><g:mi>CDM</g:mi></g:math> by assuming a higher optical depth (<j:math xmlns:j=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><j:mi>τ</j:mi><j:mo>≃</j:mo><j:mn>0.09</j:mn></j:math>), but such a value conflicts with large-scale CMB polarization data. We point out that cosmic birefringence, as suggested by recent Planck reanalyses, resolves this discrepancy if the birefringence angle varies significantly during reionization. Specifically, we consider the fact that the measured cosmic birefringence angle <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:mrow><l:msub><l:mrow><l:mi>β</l:mi></l:mrow><l:mrow><l:mn>0</l:mn></l:mrow></l:msub><l:mo>=</l:mo><l:mn>0.34</l:mn><l:mo>±</l:mo><l:mn>0.09</l:mn><l:mo stretchy=\"false\">(</l:mo><l:mn>1</l:mn><l:mi>σ</l:mi><l:mo stretchy=\"false\">)</l:mo><l:mtext> </l:mtext><l:mtext> </l:mtext><l:mi>deg</l:mi></l:mrow></l:math> has the phase ambiguity, i.e., the measured rotation angle is described by <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:mrow><p:mi>β</p:mi><p:mo>=</p:mo><p:msub><p:mrow><p:mi>β</p:mi></p:mrow><p:mrow><p:mn>0</p:mn></p:mrow></p:msub><p:mo>+</p:mo><p:mn>180</p:mn><p:mi>n</p:mi><p:mtext> </p:mtext><p:mtext> </p:mtext><p:mi>deg</p:mi></p:mrow></p:math> (<r:math xmlns:r=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><r:mi>n</r:mi><r:mo>∈</r:mo><r:mi mathvariant=\"double-struck\">Z</r:mi></r:math>). We show that cosmic birefringence induced by axionlike particles with nonzero <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mi>n</u:mi></u:math> suppresses the reionization bump, allowing a higher <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:mi>τ</w:mi></w:math> consistent with data. We provide a viable parameter space where the birefringence effect simultaneously accounts for the low-<y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mo>ℓ</y:mo></y:math> polarization spectra, the Planck E</ab:mi>B</ab:mi></ab:math> correlations, and the elevated value of <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:mi>τ</cb:mi></cb:math>, suggesting a key role for cosmic birefringence in current cosmological tensions.","PeriodicalId":20069,"journal":{"name":"Physical review letters","volume":"199 1","pages":""},"PeriodicalIF":9.0000,"publicationDate":"2025-10-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Resolving the Negative Effective Neutrino Mass Parameter with Cosmic Birefringence\",\"authors\":\"Toshiya Namikawa\",\"doi\":\"10.1103/qgnn-6hsf\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The recent measurement of baryonic acoustic oscillations by the Dark Energy Spectroscopic Instrument reveals a mild tension with observations of the cosmic microwave background (CMB) within the standard Λ</a:mi></a:math> cold dark matter (<d:math xmlns:d=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><d:mi mathvariant=\\\"normal\\\">Λ</d:mi><d:mi>CDM</d:mi></d:math>) cosmological model. This discrepancy leads to a preference for a total neutrino mass that is lower than the minimum value inferred from neutrino oscillation experiments. Alternatively, this tension can be eased within <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:mi mathvariant=\\\"normal\\\">Λ</g:mi><g:mi>CDM</g:mi></g:math> by assuming a higher optical depth (<j:math xmlns:j=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><j:mi>τ</j:mi><j:mo>≃</j:mo><j:mn>0.09</j:mn></j:math>), but such a value conflicts with large-scale CMB polarization data. We point out that cosmic birefringence, as suggested by recent Planck reanalyses, resolves this discrepancy if the birefringence angle varies significantly during reionization. Specifically, we consider the fact that the measured cosmic birefringence angle <l:math xmlns:l=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><l:mrow><l:msub><l:mrow><l:mi>β</l:mi></l:mrow><l:mrow><l:mn>0</l:mn></l:mrow></l:msub><l:mo>=</l:mo><l:mn>0.34</l:mn><l:mo>±</l:mo><l:mn>0.09</l:mn><l:mo stretchy=\\\"false\\\">(</l:mo><l:mn>1</l:mn><l:mi>σ</l:mi><l:mo stretchy=\\\"false\\\">)</l:mo><l:mtext> </l:mtext><l:mtext> </l:mtext><l:mi>deg</l:mi></l:mrow></l:math> has the phase ambiguity, i.e., the measured rotation angle is described by <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:mrow><p:mi>β</p:mi><p:mo>=</p:mo><p:msub><p:mrow><p:mi>β</p:mi></p:mrow><p:mrow><p:mn>0</p:mn></p:mrow></p:msub><p:mo>+</p:mo><p:mn>180</p:mn><p:mi>n</p:mi><p:mtext> </p:mtext><p:mtext> </p:mtext><p:mi>deg</p:mi></p:mrow></p:math> (<r:math xmlns:r=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><r:mi>n</r:mi><r:mo>∈</r:mo><r:mi mathvariant=\\\"double-struck\\\">Z</r:mi></r:math>). We show that cosmic birefringence induced by axionlike particles with nonzero <u:math xmlns:u=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><u:mi>n</u:mi></u:math> suppresses the reionization bump, allowing a higher <w:math xmlns:w=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><w:mi>τ</w:mi></w:math> consistent with data. We provide a viable parameter space where the birefringence effect simultaneously accounts for the low-<y:math xmlns:y=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><y:mo>ℓ</y:mo></y:math> polarization spectra, the Planck E</ab:mi>B</ab:mi></ab:math> correlations, and the elevated value of <cb:math xmlns:cb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><cb:mi>τ</cb:mi></cb:math>, suggesting a key role for cosmic birefringence in current cosmological tensions.\",\"PeriodicalId\":20069,\"journal\":{\"name\":\"Physical review letters\",\"volume\":\"199 1\",\"pages\":\"\"},\"PeriodicalIF\":9.0000,\"publicationDate\":\"2025-10-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical review letters\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/qgnn-6hsf\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical review letters","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/qgnn-6hsf","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
Resolving the Negative Effective Neutrino Mass Parameter with Cosmic Birefringence
The recent measurement of baryonic acoustic oscillations by the Dark Energy Spectroscopic Instrument reveals a mild tension with observations of the cosmic microwave background (CMB) within the standard Λ cold dark matter (ΛCDM) cosmological model. This discrepancy leads to a preference for a total neutrino mass that is lower than the minimum value inferred from neutrino oscillation experiments. Alternatively, this tension can be eased within ΛCDM by assuming a higher optical depth (τ≃0.09), but such a value conflicts with large-scale CMB polarization data. We point out that cosmic birefringence, as suggested by recent Planck reanalyses, resolves this discrepancy if the birefringence angle varies significantly during reionization. Specifically, we consider the fact that the measured cosmic birefringence angle β0=0.34±0.09(1σ)deg has the phase ambiguity, i.e., the measured rotation angle is described by β=β0+180ndeg (n∈Z). We show that cosmic birefringence induced by axionlike particles with nonzero n suppresses the reionization bump, allowing a higher τ consistent with data. We provide a viable parameter space where the birefringence effect simultaneously accounts for the low-ℓ polarization spectra, the Planck EB correlations, and the elevated value of τ, suggesting a key role for cosmic birefringence in current cosmological tensions.
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